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Chemical Thermodynamics of Tin - Volume 12 - OECD Nuclear ...

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274<br />

A Discussion <strong>of</strong> selected references<br />

and it was attempted to determine thermodynamic quantities <strong>of</strong> Reaction (A.18)<br />

Sn 4+ + H 2 (g) Sn 2+ + 2 H + .<br />

(A.18)<br />

The Sn 4+ /Sn 2+ electrode potential was found to be 0.154 V, which is 8 mV<br />

more positive than that given by [1914FOR/BAR].<br />

For a re-evaluation <strong>of</strong> Huey and Tartar’s measurements and the consecutive<br />

SIT analysis it is essential to convert the compositional data “Sn, mml. per 1000g. <strong>of</strong><br />

soln.” into molalities. The somewhat cryptic expression – Sn, mml. per 1000g. <strong>of</strong> soln.–<br />

has been translated into millimole (Sn) tot (SnCl 2 + SnCl 4 ) per 1000g <strong>of</strong> solution. The<br />

symbol μ and the unit mol·kg –1 has been provisionally assigned to this quantitiy. The<br />

above mentioned conversion has been based on the following relationships:<br />

1) <strong>Tin</strong> has been dissolved in HCl and partially oxidised by Cl 2<br />

μ Sn tot<br />

= μ SnCl + μ<br />

2 SnCl .<br />

4<br />

2) The molar ratio n(Sn(II))/n(Sn(IV)) can be expressed by μ or m<br />

μ SnCl 2<br />

+ μ SnCl = m<br />

4 SnCl + m<br />

2 SnCl .<br />

4<br />

3) Mass fractions can also be expressed by μ or m<br />

w SnCl 2<br />

= μ SnCl M<br />

2 SnCl /1000<br />

2<br />

= mSnCl<br />

M<br />

2 SnCl /( m<br />

2 SnCl M<br />

2 SnCl + m<br />

2 SnCl M<br />

4 SnCl + m<br />

4 HClM HCl + 1000).<br />

The column “Barometric pressure, mm at 0 °C” was treated as follows. The<br />

water activities in HCl solutions listed e.g. in Table B-1, were used to derive a quadratic<br />

function <strong>of</strong> the equilibrium vapour pressure p HO over the pertinent hydrochloric acid<br />

2<br />

solutions m HCl . The pressure <strong>of</strong> the hydrogen p H was taken as the barometric pressure<br />

2<br />

given in Table I, column 5 [1934HUE/TAR] less the calculated value <strong>of</strong> p HO.<br />

2<br />

and thus<br />

The activity coefficients <strong>of</strong> the hydrogen ion were calculated according to<br />

o<br />

m<br />

'(HCl)<br />

log10 γ ± ,HCl<br />

= − D + ε(H + , Cl – )·m HCl ,<br />

−1 −2<br />

H<br />

E = E(Sn 4+ /Sn 2+ ) − (k/2) log 10{ mSn(IV) pH m<br />

2 Sn(II) a + } was obtained.<br />

Figure A-9 shows that at m HCl ≥ 0.53 m<br />

within the scatter <strong>of</strong> the experimental data.<br />

E is independent <strong>of</strong> m (Sn)tot ,<br />

o<br />

m<br />

'(HCl)<br />

So far the results <strong>of</strong> [1934HUE/TAR] were confirmed. A problem arises,<br />

however, due to Huey and Tartar’s method <strong>of</strong> extrapolation to m HCl = 0. Probably the<br />

o<br />

o<br />

function E<br />

m<br />

'(HCl)<br />

= E<br />

m(HCl)<br />

+ b m<br />

HCl<br />

was used, although this was not stated explicitly,<br />

ο<br />

see Figure A-10. The value, E (Sn 4+ /Sn 2+ ) = 0.154 V, given by [1934HUE/TAR] has<br />

essentially been reproduced by this kind <strong>of</strong> curve fitting.<br />

CHEMICAL THERMODYNAMICS OF TIN, ISBN 978-92-64-99206-1, © <strong>OECD</strong> 20<strong>12</strong>

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